EP3959578B1

EP3959578B1 - Positionally assisted negative particle rejection (panr) to sort and enrich target cells of interest

Info

Publication number: EP3959578B1
Application number: EP20794017.2A
Authority: EP
Inventors: Steven Graves; James FREYER; Travis A. WOODS
Original assignee: Bennubio Inc
Current assignee: Bennubio Inc
Priority date: 2019-04-24
Filing date: 2020-04-24
Publication date: 2025-08-27
Anticipated expiration: 2040-04-24
Also published as: CN114556258A; AU2020262398B2; WO2020219800A1; JP7656332B2; KR20220132413A; EP3959578A1; AU2020262398A1; CA3137772A1; JP2022529490A; EP3959578A4; US20220355295A1

Description

Field of the Invention

The invention relates to systems and methods for sorting and/or enriching a target particle of interest in a fluid sample.

Background

Sorting and enrichment of desired cells and particles from a mixture is of great interest to many fields (Robinson and Roederer 2015, Shields IV, Reyes et al. 2015, Gabriel, Calleja et al. 2016). Multiparameter single cell sorting is critical to many fields, but it is too slow for many important applications [1-4]. Therefore, techniques that rapidly enrich a subset of cell types based on their physical properties (e.g. size, density, compressibility) are often used as the first step of multiparameter sorting to speed up the overall cell separation process [2, 4-6]. However, added enrichment steps increase the chance that rare cells will be lost while also increasing the complexity and cost of sorting [5]. What is needed are approaches that enable high-speed multiparameter cell and particle sorting, regardless of cell and particle size.
For the purposes of the present disclosure, the term "sorting" is intended to mean the isolation of a very specific cell or particle type on a one by one basis based on its cellular function or particle characteristics, identification of which usually requires the detection of several biological or physical markers. "Enrichment" is defined as increasing the relative concentration of a given cell or particle type as compared to the starting mixture of cells or particles. Finally, for simplicity, while the present disclosure may refer to biological "cells," it will be understood that present disclosure is equally applicable to other particles in an aqueous fluid (e.g. microspheres, multicellular aggregates, small organisms, nanoparticles (including biological nanoparticles such as viruses and prions) etc.)
Enrichment processes are fast, but do not provide high purity, as most cells have similar physical properties [2]. Enrichment steps such as the lysis of RBCs to enrich for WBCs [7] or micro-post arrays to separate WBCs[8] are successful because of the significant physical differences between RBCs and WBCs. The efficiency of such approaches makes the development of similar techniques to separate target cells indicative of disease a highly sought-after goal [9-12]. While some diseases (e.g. malaria) result in physical changes to enable efficient physical separation [6], most do not result in large enough changes of cellular properties to provide high-purity enrichment from the background cells that have a diversity in physical properties [6]. Moreover, cells of the same type can display significant physical variation from one individual cell to the next, meaning that systems that rely solely on physical properties to sort or enrich cells may identify different types of cells as being more similar than two cells of the same type.
Nonetheless, many enrichment approaches have been pursued: including deterministic lateral displacement [13-15], inertial focusing [16-20], acoustophoresis [21-23], dielectrophoresis [24-26] and a myriad of other approaches. While the label free nature and throughput of such approaches is desirable, there is no current enrichment approach that provides comparable purity to that of multiparameter sorting.
Another approach, magnetic activated cell sorting (MACS), sorts cells via the binding of magnetically tagged antibodies, followed by magnetic capture [27, 28]. MACS is fast, gentle, and high-throughput, but does not lead to high purity isolation of most rare cell types that require several cellular markers to identify. The only way to do multiparameter sorting via MACS involves sequential washing and sorting steps since each sort is binary [29].
Comparatively, fluorescently activated cell sorting (FACS) can sort cells on >20 cellular markers simultaneously [30, 31]. Using FACS, it is possible to isolate relatively rare cells (typically labelled with fluorescent antibodies) at near 100% purity in a few hours [30, 31]. These properties have resulted in FACS being the primary technology for the isolation of cellular populations [30-32]. In FACS, optical analysis is performed as the cells pass by in a flowing stream and cells of interest are labeled so that they emit light at specific wavelengths after excitation with an intense light source [32]. As many colors of fluorescence can be identified simultaneously this allows cells to be identified by the types of molecules that they are expressing or displaying, which is often the only way to differentiate different cell types [30, 31]. Each cell is identified in real time as it passes through the system and a sort signal is sent to divert cells of interest via a sort mechanism [32]. The typical sort mechanism uses a piezo drive to induce droplet formation as the high-speed fluid exits a nozzle. Only the droplets that contain the desired cells are electrostatically charged, that charge is used to divert the droplet as it passes oppositely charged plates and successfully sort the cell. The small droplet volume and high-speed timing of the FACS system enables this approach to sort at rates of up to 50,000 cells per second [32]. In contrast, recent advances in microfluidics have made it possible to, instead, use valves that open and close at 30KHz to provide nearly matching sorting rates [33, 34]. However, the use of hydrodynamic focusing and/or microfluidics in these commercial systems typically presents as flow rates <100 mL/min for sample delivery, which precludes sorting of large volume samples. Therefore, pre-enrichment steps are used prior to flow sorting for rare cell populations. Unfortunately, such steps add complexity, require additional processing time, and lead to loss of rare cells - all of which are highly problematic for rare cell isolation from large volume samples.
For particles larger than single cells (i.e. >50 mm in diameter) the choice of sorting technology becomes even more restrictive. Large particle sorting technology exists and is similar to the FACS approach described above, but sorting is accomplished using a puff of air to displace a flowing jet in air stream [35, 36]. Due to limitations with hydrodynamic focusing of larger particles and the relatively slow sort mechanism, this approach is limited to sorting of about 100 particles per second at ~200 mm diameter and even slower for larger particles.
For the above reasons, creation of approaches to accurately isolate cells and other particles in simple, fast, and gentle fashion remains a significantly valuable challenge to be overcome. Most of the proposed improvements have pursued microfluidic solutions and there are many commercially available microfluidic cell sorters [37]. Nonetheless, the volumetric rate of cell sorting is limited to about 100 µl/min with an effective sorting rate of about 50K cells/sec (and much lower for larger particles). This is a serious limitation for sorting large numbers of rare cells (e.g. stem cells for therapy) because these approaches cannot analyze enough sample in a reasonable time to produce a large yield of the rare cell population.
Despite this research and commercial development, the basic limits of fluorescent activated cell sorting remain. Most current approaches use microfluidics and extremely fast valves to ensure that each sort step is as fast as possible and that the smallest sort volume possible is used. This approach is inherently limited to sort rates of about 50,000 events per second due to the stochastic arrival of particles and the rapid increase in system pressure as linear velocity increases.
Because of such limitations, alternative sorting approaches have been considered. For example, Ensemble-decision aliquot ranking (EDAR) uses a laser to generate fluorescence signal from many cells in an aliquot of sample within a microfluidic channel, which dramatically reduces its ability to resolve true positive signals from that generated by background binding of multiple antibody types to cells coincident in the aliquot [38, 39]. Following analysis, the aliquot flows into a junction that provides input buffer from both sides to focuses the flowing aliquot of cells into the central channel of three exit channels. Using solenoid valves to control the flow of input buffer enables EDAR to sort aliquots to either of the side exit channels. Beyond EDAR, there have been many other approaches including: piezoelectric drives to switch flows or cells [40-42], lasers to move cells [43]. All of these approaches are limited by throughput and sorting rates.
WO2018/148194 describes a system to detect and characterize individual particles and cells using at least either optic or electric detection as the particle or cell flows through a microfluidic channel. The system also provides for sorting particles and cells or isolating individual particles and cells.
Accordingly, there remains a need for systems that are able to quickly and accurately sort and/or enrich for desired cells in a mixed sample or population.

Summary

The present disclosure provides novel methods and systems for sorting and enriching target cells of interest from a mixture, as set out in the claims.

Brief Description of the Drawings

Fig. 1 is a schematic illustration of a PANR system according to an embodiment of the present disclosure.
Figs. 2A-2E are schematic illustrations of a non-limiting exemplary device in use to detect, sort, and enrich for target cells of interest.
Fig 2A shows cells being positioned by an acoustic standing wave produced by a PZT drive.
Fig. 2B shows a cell of interest arriving in the interrogation area.
Fig. 2C shows a signal being generated by the detection system such and the rejection channel valve closing.
Fig. 2D shows the cell of interest having flowed into the collection channel and the rejection channel valve opening.
Fig. 2E shows the system having reverted to the open valve state.
Fig. 3 is a flow diagram showing repeated PANR according to an embodiment of the present disclosure.
Fig. 4 depicts the concentration in the collection channel (Cc) as a function of target cell concentrations (C ₊) and background cell concentrations (C_- ).
Fig. 5 depicts the Volume (VC) in the collection channel as a function of target cell concentration (C₊) and background cell concentration (C_-).
Fig. 6 depicts fractional purity in the collection channel as a function of target cell concentration (C+) and background cell concentration (C-). For situations where C+ is >> C-the fractional purity will go higher than 1 as there will be more than 1 target cell in each sort. This situation is not plotted here.

Detailed Description

According to an embodiment the present disclosure provides novel methods and apparatus for sorting and enriching target particles of interest from a mixture. According to various embodiments described below, the novel methods and apparatus for sorting and enriching target particles of interest are referred to as Positionally Assisted Negative particle Rejection (PANR).
Fig. 1 is a schematic illustration of a PANR system according to an embodiment of the present disclosure. In general, system 10 includes a flow channel 12 which is partitioned at the distal end to produce a collection channel 14 and a rejection channel 16. The intended flow direction is shown with arrow 18. (For clarity, in the present disclosure, the terms proximal and distal are used with reference to the intended direction of flow within the device during standard operation such that a fluid sample typically flows from the proximal end to the distal end of a channel.) The proximal end of channel 12 includes a particle positioning/focusing device 20. The particle positioning device positions (or focuses) particles within channel 14. In PANR, particle positioning accomplishes at least two tasks: first, each particle is positioned so that it can be interrogated by detector 22, second, each particle is positioned so that it will flow, by default, through rejection channel 16. Detector 22 is in communication with valve 24.
In operation, particles in a sample are introduced at the proximal end of the collection channel, where they are positioned (or focused) by device 20. Device 20 may be, for example, any device capable of positioning the particles to accomplish the tasks identified above. Suitable devices include apparatus capable of producing acoustic standing waves such as a piezoelectric transducer (PZT) drive. Other devices or positioning methodologies that could be employed include, but are not limited to, micropost arrays for deterministic lateral displacement, inertial focusing, and dielectrophoretic focusing. Additionally, methods of positioning that require the addition of fluid, such as hydrodynamic focusing, would also work as long as all of the additional fluid was accounted for in the calculations and the approach.
After being focused, the particles are interrogated by detection device 22. In general, detection device 22 is capable of distinguishing a single or very few particles of interest from background particles. (See, e.g., ref 44-48) According to a specific embodiment, detection device 22 includes a focused light source such as a laser and an optical detector. In this embodiment, once the particles are positioned, they flow through interrogation zone 26 where they encounter the focused light and emit optical signals that are analyzed by the optical detector, which determines whether any particular particle is a particle of interest. Of course it should be understood that while optical signal detection is shown, any method of interrogating the cell (imaging, ultrasound, etc.) would work as long as it can identify the particle of interest and provide a signal when a particle of interest is detected.
Detection device 22 is then in communication with valve 24. In normal operation, when no particle of interest is detected, valve 24 is open and the sample fluid flows out of the detection channel and through rejection channels 16 and collection channel 14. Importantly, positioning device 20 has specifically positioned all the particles within channel 12 such that any particles in the detection channel will naturally flow through rejection channel 16 (this may also be referred to as a discard, or discharge channel), even while a smaller volume of fluid (without particles) flows into the collection channel 14.
In contrast, when detection device 22 identifies a particle of interest, it sends a signal to valve 24 to close the valve, which redirects particles within the interrogation zone towards and out through collection channel 14. As shown by dotted arrow 28, collected particles of interest (and any background stragglers) are recirculated back to the proximal end of the device for one or more additional rounds of sorting/enrichment.
The channels and valves may formed from standard materials commonly used in fluidic and microfluidic industries and may be manufactured using standard techniques including, but not limited to micromachining, microlithography, etching, 3D printing, etc. [50] Suitable solenoid valves can be manufactured or are commercially available. For example, suitable commercially available solenoid valves having 200 µs response times are available from TLX Technologies (Pewaukee, WI).
While Fig. 1 depicts a single flow channel, which enables automatic recirculation of the collected particles of interest, as explained in greater detail below, the present disclosure contemplates arrangements wherein multiple flow channels are used in parallel and/or in sequence in order to process large sample volumes quickly. It will also be understood that such multi-channel arrangements could be designed to detect and collect one or more types of particles of interest. Moreover, more than one type of particle of interest could be identified as a particle of interest by detection device 22. Accordingly, in various embodiments, the presently described system could be designed to identify and collect more than one specific type of particle - simultaneously (i.e. within the same flow channel), in parallel (i.e. within multiple flow channels operating at the same time) or in sequence (i.e., a first pass detects one type of particle while a second pass detects another type of particle.)
Figure 2A-2E are schematic illustrations of a non-limiting exemplary device in use to detect, sort, and enrich for target cells of interest. In the depicted embodiment, a fluid sample containing both background cells (dark circles) and target cells of interest (light circles) enters at the left (proximal end) of the channel and flow to the right, as shown by the arrow. Fig. 2A shows the cells being positioned by an acoustic standing wave produced by a PZT drive. Once the cells have been positioned, they flow through the laser beam and emit optical signals that are analyzed by the detector. Determination of whether a particular cell is of interest is made by analysis of emitted optical signals. As shown, so long as only background cells are detected, the rejection channel valve is open and all the cells flowing through the device exit via the rejection channel, while a small amount of fluid (without cells) flows through the collection channel. In this "open valve" state, and as explained in greater detail below, the volume of fluid that is directed through a given channel is determined by the relative cross-sectional area of the channel opening to the total area of the channel.
Of course it will be understood that Figs. 2A-2E only show one example of multiple possible various design configurations, including, for example single- or multi-valve designs where fluid only flows through the collection channel after a cell of interest is identified.
Returning to the configuration shown in Figs. 2A-2E, if a cell of interest arrives in the interrogation area (Fig. 2B), a signal is generated by the detection system that triggers the valve on the rejection channel to close (Fig. 2C). In this "closed valve" state, the flow of the rejection channel is stopped, which forces all flow through the open collection channel. As all flow is forced through the collection channel, all cells and all fluid will be directed through the collection channel. After the cell of interest is predicted to have flowed into the collection channel, the valve begins to open (Fig. 2D) and the system reverts back to the open valve state (Fig. 2E).
In this way, all cells of interest are collected into the collection channel. Of course, if the valve is in the closed state long enough background cells are also collected. However, if the target cells are relatively rare as compared to the background cells (discussed in detail below), most background cells will be diverted to the rejection channel and all target cells will be retained in the collection channel. This will result in an effective enrichment of the number of target cells relative to background cells.
Intuitively it can be seen that this process will result in numerical enrichment of cells of interest and that repeated use of this approach (i.e. passing the collected volume back through the system) will eventually result in only target cells of interest in the collection channel. Thus, initial passages through the system will result in target cell enrichment and repeated passages will result in an effective sorting process, where target cells of interest are the only remaining cells in the collection volume. Of course, at the end of repeated processes the target cells may be at a low concentration in a large volume, but, at that point, very simple cell concentration techniques such as centrifugation or acoustophoresis can be used to collect the cells at any concentration necessary.
Accordingly, use of repeated PANR (referred to herein as rPANR) will result in effective sorting of cells of interest. Fig. 3 is a flow diagram showing this approach.
The system and methods of the present disclosure maximize the fluidic throughput of the system while emphasizing total sample recovery to enable multiple cycles of a fast fractionation of target cells. The target cells are recovered in their natural sample background for additional sorting steps that can occur rapidly. As described below, this paradigm shift will enable rPANR to sort cells from samples as large as a liter and for target cells as rare as 1 per liter in a background of 10⁷ negative cells in automated fashion and in a few hours. Moreover, this process will be somewhat unaffected by particle size. These sort rates are simply not achievable using any other approach and will have great significance in rare cell sorting, high-throughput cell sorting, and large particle sorting. As such, rPANR will be of great value across all aspects of biomedical and clinical research as well as for therapy-scale cell separations.
The PANR process can be described in a series of equations to mathematically model the rPANR process. Equation 1 calculates the delay volume (V_D ), which is the sample volume that will pass through the collection channel due to the valve closing, where F is the volumetric flow rate (F), flt is the time it takes the valve to open and close. $V_{D} = F \cdot Δ t$
Thus, the faster the valve the smaller this volume will be, which will enable a higher enrichment on an individual PANR passage as fewer nonspecific background cells will be present in the V_D. Equation 2 calculates the fraction of the total channel cross-sectional area that the collection channel makes up (U), where xArea collection is the cross-sectional area of the collection channel and xArea rejection is the cross-sectional area of the rejection channel. $U = \frac{xArea collection}{xArea collection + xArea discharge}$
Equation 3 calculates the number of delay volumes that will cause to close (Y), where C ₊ is the concentration of target cells, C_- is the background cell concentration, and V_T is the total sample volume. $Y = (1 - e^{- C_{+} \cdot V_{D}} \cdot \frac{{(- C_{+} \cdot V_{D})}^{0}}{0!}) \cdot \frac{V_{T}}{V_{D}} = \frac{V_{T}}{V_{D}} \cdot (1 - e^{- C_{+} \cdot V_{D}})$
Equation 4 calculates the number of delay volumes where the valve is open (N) where N is calculated by simply subtracting Y from the total number of times the valve can open or close, which is V_T / V_D. $\begin{matrix} N = \frac{V_{T}}{V_{D}} - Y = \frac{V_{T}}{V_{D}} - (1 - e^{- C_{+} \cdot V_{D}}) \cdot \frac{V_{T}}{V_{D}} = \frac{V_{T}}{V_{D}} \cdot (1 - (1 - e^{- C_{+} \cdot V_{D}})) \\ = \frac{V_{T}}{V_{D}} \cdot e^{- C_{+} \cdot V_{D}} \end{matrix}$
Using these constants, we calculate system variables for specific model conditions. For example, Equation 5 calculates the volume that flows into collection channel (V_C ) during a single cycle of PANR, where we count the number of times the valve is open (Y) and multiply that by the delay volume (V_D ). $V_{C} = Y \cdot V_{D} + N \cdot U \cdot V_{D} = V_{D} \cdot (Y + N \cdot U)$
We also add the volume that passes to the collection channel while the valve is open, which is the number of times that the valve is open (N) multiplied by V_D, corrected for the fraction of the volume that will pass through the collection channel (U) during the open valve state. Substituting Equations 3 and 4 into Equation 5, provides Equation 6, which calculates the volume expected to flow into the collection channel based on the total volume of the sample (V_T ). $\begin{matrix} V_{C} = V_{D} \cdot (\frac{V_{T}}{V_{D}} \cdot (1 - e^{- C_{+} \cdot V_{D}}) + \frac{V_{T}}{V_{D}} \cdot e^{- C_{+} \cdot V_{D}} \cdot U) \\ = V_{T} ((1 - e^{- C_{+} \cdot V_{D}}) + U \cdot e^{- C_{+} \cdot V_{D}}) \end{matrix}$
We can also calculate the number of cells that end up in the collection channel (P_c ) as shown in Equation 7, which is valid for low target cell concentrations and calculates the number of background cells as the number of valve closings (Y) added to the average number of background cells in a V_D. $P_{c} = Y + Y \cdot \frac{C_{-}}{V_{D}}$
As target cell concentrations increase, it becomes more likely that more than one cell will be present in a V_D. As such, this model is valid for low target cell concentrations (e.g. C+:50.2 cells per V_D, which provides a 98.2% chance of 1 or fewer target cells per V_D ). By substituting Equation 3 into Equation 7, Equation 8 calculates P_c , using known parameters. $\begin{matrix} P_{c} = Y + Y \cdot C_{-} \cdot V_{D} = \frac{V_{T}}{V_{D}} \cdot (1 - e^{- C_{+} \cdot V_{D}}) + \frac{V_{T}}{V_{D}} \cdot (1 - e^{- C_{+} \cdot V_{D}}) \cdot C_{-} \cdot V_{D} \\ = \frac{V_{T}}{V_{D}} \cdot (1 - e^{- C_{+} \cdot V_{D}}) \cdot (1 + C_{-} \cdot V_{D}) \end{matrix}$
Equation 9 combines Equations 6 & 8 to calculate the concentration of cells in the collection channel (C_c ). $\begin{matrix} C_{C} = \frac{P_{C}}{V_{C}} = \frac{\frac{V_{T}}{V_{D}} \cdot (1 - e^{- C_{+} \cdot V_{D}}) \cdot (1 + C_{-} \cdot V_{D})}{V_{T} ((1 - e^{- C_{+} \cdot V_{D}}) + U \cdot e^{- C_{+} \cdot V_{D}})} \\ = \frac{(1 - e^{- C_{+} \cdot V_{D}}) \cdot (1 + C_{-} \cdot V_{D})}{V_{D} ((1 - e^{- C_{+} \cdot V_{D}}) + U \cdot e^{- C_{+} \cdot V_{D}})} \end{matrix}$
Finally, our model can determine purity as a function of the number of total target cells of interest (P ₊) divided by the number of cells present in the collection channel (P_c ), as shown in equations 10 & 11. Equation 10 calculates P ₊ simply by multiplying the known target cell concentration times the total sample volume (V_T ) at the start of the process.
Using equations 8 and 10 enables the fractional cell purity (Purity) to be calculated (Equation 11). $\begin{matrix} Purity = \frac{P_{+}}{P_{C}} = \frac{C_{+} \cdot V_{T}}{\frac{V_{T}}{V_{D}} \cdot (1 - e^{- C_{+} \cdot V_{D}}) \cdot (1 + C_{-} \cdot V_{D})} \\ = \frac{C_{+} \cdot V_{D}}{(1 - e^{- C_{+} \cdot V_{D}}) \cdot (1 + C_{-} \cdot V_{D})} \end{matrix}$
This model enables useful predictions using real-world parameters, such as the effect of valve response time on V_D in a constructible system. As there are commercially available miniature solenoid valves with 200 µs response times (TLX Technologies, Pewaukee, WI), we can assume flt of 1 ms, which includes the time to send a sort signal to the valve. Using a flow rate (F) of 1 mL/min or 167 µL/s, V_D would be 17 nL. A C ₊ of 1cell per 5x the V_D (85 nL), which is <1.2x10⁴ target cells/ml, ensures the required low cell concentration for our model. At higher C+, more than one target cell may be coincident in V_D. In a conventional sorter, this would be problematic, but in PANR operation, within some limitations, it will result in more efficient enrichment as a greater proportion of target cells would be present in the collection channel. However, our model assumes that the valve is mostly open. Thus, the limitation of the system is driven by how often the volume equivalent to V_D preceding the V_D being sorted contains a target cell. If the preceding V_D is occupied by a target cell, the valve will remain closed. Again, Poisson statistics suggest that, at 1.2x10⁴ target cells/ml, 82% of the time the 17 nL volume preceding the 17 nL V_D being sorted will be clear of target cells. In fact, at concentrations as high as 6x10⁴ target cells/mL, the preceding V_D be clear of target cells 50% of the time, which is likely to be near the limit where PANR will be operational. With regards to the size of the fluidic channels, if we use a 100 µm x 100 µm square channel as the lower dimensional limit, this channel would be 1.7 mm long to contain 17 nL. If one considers a system that positions cells to a line and assumes the cells are 10 µm in diameter, this limits the concentration of cells to 170/17 nL if they are packed as beads on a string, which results in a maximum total cell concentration of 1 x 10⁷ cells/ml. If acoustic cytometry is being used, at these concentrations one would expect to see some coincidences during analysis [49], but it should not be inherently limiting to the optical analysis approach.
Fig. 4 examines the concentration in the collection channel (Cc) as a function of target cell concentrations (C+) and background cell concentrations (C_- ). As can be seen by this plot, starting at high cell concentrations (10⁴ target cells/ml & 10⁷ background cells/ml) leads to marginal improvement using this approach. In fact, the expected concentration only improves from 10⁴/10⁷ to 10⁴/7.6x10⁶, which is ~24% enrichment in terms of concentration (i.e. a 24% reduction of background cells). The impact improves as the starting target cell concentration decreases. Starting at 10³ and 10⁷, results in an enrichment of 83%, and 10² and 10⁷ provides an enrichment of 98%. Fig. 5 shows that use of 10⁴ target cells results in a ~7.3 mL volume being directed to the collection channel, while 10³ provides ~4.5mL, and 10² starts to approach 4 mL. This is consistent with the fractional volume collected in the model (40%) and the starting volume (10mL). Fig. 6 examines the total purity of the cells in terms of cell count (positive cells/total cells) it can be seen that starting with 10⁴ positive cells in 10⁷ background cells, only results in an improvement in cell purity of 0.13%, it remains relatively constant even as target cell concentration is reduced (0.12% for 103/mL and 102/mL). However, as the relative starting target cell concentration becomes nearer the background cell concentration (e.g. 10⁴ and 10⁶ cell/mL respectively) this situation dramatically improves by a factor of 10. As the starting background cell concentration decreases to 10⁵ to 10⁴ cells/ml, the ability to achieve a fractional purity of 1 for target cells of interest is clear for target cell populations at concentrations of <10⁴ cells/ml.
According to an embodiment, the presently described rPANR process can be implemented with a parallel acoustic flow cytometry system, such as the commercially available Velocyt^™ system (BennuBio, Inc. Albuquerque, NM) which can analyze cell samples at high concentrations, at analysis rates of 2x105 cells/s, and at flow rates of 10 mL/min [48]. Such an instrument can analyze 10-15 parallel streams of cells in a variety of flow cell configurations and eventually provide up to 16 optical parameters. By implementing rPANR in a parallel acoustic flow cytometry system, the presently described methods can be used to pursue sorting with target cell concentrations of between 10^-3 to 10⁴ target cells/mL from a concentration of 107 background cells/mL. Current sorters require pre-enrichment steps to sort such samples. Figure 4 considers the use of a 10 stream Velocyt instrument as the basis for an rPANR process and extrapolates how it compares to conventional flow sorting with a pre-enrichment step.
According to various other embodiments the presently described detection systems and methods can provide multiparameter analysis of each cell. This can simply be multiparameter fluorescent analysis, index of refraction, or scatter where the cell is identified via the optical signal generated by one or more lasers. Additionally, other parameters such as cellular impedance, ultrasound response, or others could be combined to provide a sort signal based on the analysis of multiple cellular properties.
The terms and expressions that have been employed are used as terms of description and not of limitation, and there is no intent in the use of such terms and expressions to exclude any equivalent of the features shown and described or portions thereof, but it is recognized that various modifications are possible within the scope of the invention as claimed. Thus, it will be understood that although the present invention has been specifically disclosed by preferred embodiments and optional features, modification and variation of the concepts herein disclosed may be resorted to by those skilled in the art, and that such modifications and variations are considered to be within the scope of this invention as defined by the appended claims.
All patents and publications referenced below and/or mentioned herein are indicative of the levels of skill of those skilled in the art to which the invention pertains.

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Claims

A system (10) for sorting and/or enriching a target particle of interest in a fluid sample comprising:
a flow channel (12) having an interrogation zone (26) and an end that bifurcates into a collection channel (14) and rejection channel (16), wherein the rejection channel (16) comprises a valve (24);

a positioning device (20) adapted to position particles in the flow channel (12) such that when the valve (24) is open, the particles in the flow channel (22) will flow into the rejection channel (16) but not into the collection channel (14);

a detection device (22) adapted to interrogate particles within the interrogation zone (26), wherein the detection device (22) is in communication with the valve (24);

wherein detection of a target particle of interest within the interrogation zone (26) by the detection device (22) results in the valve (24) closing, forcing the target particle of interest and all fluid in the channel to flow into the collection channel (14),

wherein a portion of the fluid sample not comprising particles flows into the collection channel (14) when the valve (24) is open,

wherein the collection channel (14) is fluidly connected to an inlet that returns the flow containing collected particles to the flow channel (12) upstream from the interrogation zone (26).
The system of claim 1 wherein the positioning device (20) uses an acoustic standing wave to position the particles in the flow channel (12), or
wherein the positioning device (20) uses inertial focusing to position the particles in the flow channel (12).
The system of claim 1 wherein the positioning device (20) uses dielectrophoretic focusing to position the particles in the flow channel (12).
The system of claim 1 wherein the positioning device (20) is a piezoelectric transducer.
The system of claim 1 wherein the detection device (22) is an optical detection device.
The system of claim 1 wherein the detection device (22) includes a laser beam through which the particles pass and the detection device (22) detects optical signals emitted by the particles.
The system of claim 1 wherein the detection device (22) uses imaging to detect the particle of interest, or wherein the detection devices uses ultrasound to detect the particle of interest.
The system of claim 1 further comprising a series of flow channels so as to interrogate multiple samples in parallel.
A method for sorting or enriching a target particle of interest in a fluid sample comprising:
providing a Positionally Assisted Negative particle Rejection (PANR) system (10) comprising:
a flow channel (12) having an interrogation zone (26) and an end that bifurcates into a collection channel (14) and rejection channel (16), wherein the rejection channel (16) comprises a valve (24);

a positioning device (20) that positions particles in the flow channel (12) such that when the valve (24) is open, the particles in the flow channel (12) will flow into the rejection channel (16) but not into the collection channel (14);

a detection device (22) that interrogates particles within the interrogation zone (26), wherein the detection device (22) is in communication with the valve (24);

wherein detection of a target particle of interest within the interrogation zone (26) by the detection device(22) results in the valve (24) closing, forcing the target particle of interest to flow into the collection channel (14);

delivering the fluid sample to the flow channel (12 )for interrogation and collection; and

collecting the contents of the collection channel (14),.
further comprising delivering the collected contents of the collection channel (14) back to the flow channel (12) and performing subsequent rounds of interrogation and collection until a desired level of sorting and/or enrichment has been reached.
The method of claim 9 further comprising concentrating the collected particles.
The method of claim 9 wherein the particles of interest are cells, or
wherein the particles of interest are multicellular aggregates, or

wherein the particles of interest are small organisms, or

wherein the particles of interest are nanoparticles.
The method of claim 9 wherein the particles are microspheres or nanospheres.